4.7 Article

Scaling theory for vortices in the two-dimensional inverse energy cascade

期刊

JOURNAL OF FLUID MECHANICS
卷 811, 期 -, 页码 742-756

出版社

CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2016.756

关键词

turbulence simulation; turbulence theory; vortex dynamics

资金

  1. Fields Institute
  2. Natural Environment Research Council [NE/M014983/1]
  3. NERC [NE/M014983/1] Funding Source: UKRI
  4. Natural Environment Research Council [NE/M014983/1] Funding Source: researchfish

向作者/读者索取更多资源

We propose a new similarity theory for the two-dimensional inverse energy cascade and the coherent vortex population it contains when forced at intermediate scales. Similarity arguments taking into account enstrophy conservation and a prescribed constant energy injection rate such that E similar to t yield three length scales, l(omega,) l(E) and l(psi), associated with the vorticity field, energy peak and streamfunction, and predictions for their temporal evolutions, t(1/2), t and t(3/2), respectively. We thus predict that vortex areas grow linearly in time, A similar to l(omega)(2)similar to t, while the spectral peak wavenumber k(E) 2 pi l(E)(-1) similar to t(-1) We construct a theoretical framework involving a three-part, time-evolving vortex number density distribution, n(A) similar to t(alpha i)A(-ri), i is an element of 1, 2, 3. Just above the forcing scale (i= 1) there is a forcing-equilibrated scaling range in which the number of vortices 2 at fixed A is constant and vortex 'self-energy' E-v(cm)= (2D)(-1)integral omega(2)(v)A(2)n(A) dA is conserved in A-space intervals [mu A(0)(t), A(0)(t)] comoving with the growth in vortex area, A(0)(t) similar to t. In this range, alpha(1)= 0 and n(A) similar to A(-3). At intermediate scales (i =2) sufficiently far from the forcing and the largest vortex, there is a range with a scale-invariant vortex size distribution. We predict that in this range the vortex enstrophy Z(v)(cm) = (2D)(-1)integral omega(2)(v)An(A)dA is conserved and n(A) similar to t(-1)A(-1). The final range (i = 3), which extends over the largest vortex-containing scales, conserves sigma(cm)(v) = (2D)(-1)integral omega(2)(v)n(Lambda) dA. is constant in time, this is equivalent to conservation of vortex number N-v(cm) = integral n(A) dA. This regime represents a 'front' of sparse vortices, which are effectively point-like; in this range we predict n(A) similar to t(r3-1)A(-r3). Allowing for time-varying omega(2)(v) results in a small but significant correction to these temporal dependences. fligh-resolution numerical simulations verify the predicted vortex and spectral peak growth rates, as well as the theoretical picture of the three scaling ranges in the vortex population. Vortices steepen the energy spectrum E(k) past the classical k(-5/3) scaling in the range k is an element of [kf,k(v)] kull, where k, is the wavenumber associated with the largest vortex, while at larger scales the slope approaches -5/3. Though vortices disrupt the classical scaling, their number density distribution and evolution reveal deeper and more complex scale invariance, and suggest an effective theory of the inverse cascade in terms of vortex interactions.

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